srf development for high energy physics · tristan and kekb tristan was an electron-positron...
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SRF Development for
High Energy Physics Mark Champion
SRF 2011
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Introduction
• The HEP community has shown increasing
interest in SRF technology in recent years
ILC R&D program
Project X at Fermilab
Neutrino factories and muon colliders
• However, the application of SRF technology to
HEP research has a long history
• Now let’s go back in time and take a look at
that history
2 Mark Champion – SRF 2011
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Stanford High Energy Physics Laboratory (HEPL)
a.k.a. Hanson Experimental Physics Laboratory
• 1962: First measurements of superconducting cavity
performance
Lead-plated S-band 2856 MHz muffin tin cavities
Qo ~ 1e8-1e9, Bp ~ 100 G (10 mT), 4 K
• 1965: First acceleration of electrons with a
superconducting cavity
• 1972: First superconducting accelerator
Based on L-band 1300 MHz niobium cavities
Cavity performance limited by multipacting
the elliptical cavity shape was not yet developed
3 Mark Champion – SRF 2011
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HEPL 1300 MHz Cryomodule Pair
4 Courtesy of T. Smith, HEPL Mark Champion – SRF 2011
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Layout of HEPL Cryomodule
55 cell, 1300 MHz,
bi-periodic structure
~2.5 MeV/m
5 Mark Champion – SRF 2011
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TRISTAN and KEKB
TRISTAN was an electron-positron collider constructed at
KEK in the 80’s
• 32 five-cell 508 MHz elliptical SC cavities housed in 16
cryomodules
• Installed in 1988 – 1989 (augmented existing NC cavities)
• Eacc = 5 MV/m, Qo = 2e9 at 4.2 K, continuous wave
• TRISTAN was shut down in 1995
KEKB was an asymmetric-energy electron-positron collider
constructed at KEK in the 90’s
• Reused much of the TRISTAN infrastructure and components
• 8 single-cell 508 MHz SC cavities housed in 8 cryomodules
• Ecavity = 1.2 – 2 MV, Qo ~ 1e9 at 4.2 K, continuous wave
• Heavy beam loading and HOM loading ( IB = 1.4 A )
• KEKB has been shut down and is being upgraded to SuperKEKB
6 Mark Champion – SRF 2011
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http://accelconf.web.cern.ch/accelconf/SRF89/papers/srf89g29.pdf
Cryostat for TRISTAN SRF Cavities
7 Courtesy of N. Toge, KEK Mark Champion – SRF 2011
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From KEK Annual Report 1988 - http://www-lib.kek.jp/ar/ar.html
Cryomodules in the TRISTAN MR Tunnel
8 Courtesy of N. Toge, KEK Mark Champion – SRF 2011
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http://epaper.kek.jp/p99/PAPERS/THBL2.PDF
Cryostat for KEKB SRF Cavities
9 Courtesy of N. Toge, KEK Mark Champion – SRF 2011
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• KEK Annual Report 1998 - http://www-lib.kek.jp/ar/ar.html
• http://www-acc.kek.jp/kekb/pictures/KEKB_photo/ring1.jpg
Cryomodules in the KEKB Tunnel
10 Courtesy of N. Toge, KEK
Mark Champion – SRF 2011
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DESY HERA 500 MHz Cryomodules
• Electron-proton collider
• 16 SC cavities commissioned in
electron storage ring in 1991-1992 Augmented 84 NC 500 MHz cavities to
increase beam energy
• Bulk niobium, RRR 300, 4-cell,
500 MHz elliptical cavities
• Eacc = 5 MV/m, Qo = 2e9 at 4.2 K,
continuous wave
• Two klystrons, combined, drive all 16
cavities (vector sum RF control)
• HERA experiment concluded in 2007
• The initiation of the TESLA Test
Facility coincided approximately with
the successful commissioning of the
HERA SC cavities
11 Courtesy of W-D Moeller, DESY Mark Champion – SRF 2011
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HERA Cavities and Cryomodule
12 Courtesy of W-D Moeller, DESY Mark Champion – SRF 2011
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LEP Superconducting Cavities
• The LEP electron-positron collider at CERN was
upgraded with SC cavities in the period 1992-
1999
• Beam energy increased from ~46 GeV to
~100 GeV
• Final configuration: 288 four-cell cavities
272 niobium sputtered onto copper cavities
16 bulk niobium cavities
48 copper cavities (originally 128)
• 352 MHz, 4.5 K, continuous wave
• 8 cavities per 1.3 MW klystron
• LEP cryomodules were removed in 2000-2001
to make way for the LHC
13 Mark Champion – SRF 2011
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LEP 352 MHz Cavity and Cryomodule
14
Courtesy of CERN
4 cavities / cryomodule
72 modules going into storage Mark Champion – SRF 2011
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Achieved Gradients in LEP Cu/Nb Cavities in 1999
15 P. Brown et al., “Performance of the LEP200
Superconducting RF System,” SRF1999.
Highest performance achieved at end of run
• Operated cavities near their limits
• Increased limits via RF conditioning
• < Eacc > ~ 7.2 MV/m
• Qo ~ 3e9 at operating gradient
Mark Champion – SRF 2011
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LHC Superconducting Cavities
• 400 MHz, single-cell, niobium sputtered onto
copper cavities, 4.5 K, continuous wave
• Four cavities per cryomodule
• Sixteen cavities total
• 2 MV / cavity (5.3 MV/m), Qo > 1e9
• One klystron per cavity
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LHC SC Cavity
Mark Champion – SRF 2011 17
P. Maesen, “LHC Superconducting Cavities,” CWRF2008
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LHC Cryomodule
Mark Champion – SRF 2011 18 Courtesy of CERN
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CESR – Cornell Electron Storage Ring
• Electron-positron collider completed in 1979
• Upgraded with four SC cavities in the period
1997 – 1999 (replaced NC cavities)
500 MHz, single-cell, one cavity per cryomodule
Eacc = 6 MV/m, Qo > 1e9 at 4.2 K, continuous wave
Heavy beam loading and
HOM loading ( IB ~ 0.8 A max)
Cavity and Cryomodule
design was industrialized
with Accel (now RI) and
sold to several light sources
world wide
AES is presently fabricating two
of these systems
19 Mark Champion – SRF 2011 Courtesy of Cornell University
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CESR-B 500 MHz Cryomodule
20 Mark Champion – SRF 2011 Courtesy of Cornell University
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Future HEP Applications of SRF Technology
• International Linear Collider
Approximately 17,000 cavities over 31 km
• Project X
3 GeV continuous-wave H- linac followed by 8 GeV
pulsed H- linac
• Large Hadron Collider upgrades
Crab cavities for interaction region
• Muon Collider / Neutrino Factory
Project X driver plus downstream acceleration of
muon beam
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International Linear Collider Layout
Mark Champion – SRF 2011 22
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ILC Cavities and Cryomodules
Each cryomodule contains (8 cavities + 1 magnet) or (9 cavities)
Total ~2000 cryomodules, ~17000 cavities.
23 Mark Champion – SRF 2011
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Project X Reference Design
Mark Champion – SRF 2011 24
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PX SRF Linac Technology Map
25
b=0.11 b=0.22 b=0.4 b=0.61 b=0.9
325 MHz
2.5-160 MeV
b=1.0
1.3 GHz
3-8 GeV
ILC
650 MHz
0.16-3 GeV
Section Freq Energy (MeV) Cav/mag/CM Type
SSR0 (bG=0.11) 325 2.5-10 18 /18/1 SSR, solenoid
SSR1 (bG=0.22) 325 10-42 20/20/ 2 SSR, solenoid
SSR2 (bG=0.4) 325 42-160 40/20/4 SSR, solenoid
LB 650 (bG=0.61) 650 160-460 36 /24/6 5-cell elliptical, doublet
HB 650 (bG=0.9) 650 460-3000 160/40/20 5-cell elliptical, doublet
ILC 1.3 (bG=1.0) 1300 3000-8000 224 /28 /28 9-cell elliptical, quad
CW Pulsed
Mark Champion – SRF 2011 Courtesy of Bob Kephart, Fermilab
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26 Mark Champion – SRF 2011 Courtesy of S. Geer, Fermilab
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Summary
• HEP has been a driver for the development of SRF
technology for many years
Starting at Stanford in the early 60’s
Successful implementation at HERA, CESR, TRISTAN,
KEKB, LEP, and LHC
• HEP has continued this role in recent years with the ILC
R&D program and Project X
• HEP plans for future accelerators require SRF
technology
ILC, Project X, LHC upgrades, and Muon collider / Neutrino
factory
• Substantial overlap with non-HEP applications is driving
collaborations world wide
Spallation neutron sources, nuclear physics, light sources,
and Accelerator Driven Systems
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Acknowledgements
• Thanks to all of the colleagues in the SRF
community for 50 years of effort to develop and
utilize SRF technology
• Thanks for the many publications, from which I
have obtained the information for this
presentation
• Special thanks to Wolf-Dietrich Moeller, Todd
Smith, and Nobu Toge
28 Mark Champion – SRF 2011